JP2890863B2 - Polarization method for block-shaped piezoelectric material - Google Patents

Polarization method for block-shaped piezoelectric material

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Publication number
JP2890863B2
JP2890863B2 JP3298491A JP3298491A JP2890863B2 JP 2890863 B2 JP2890863 B2 JP 2890863B2 JP 3298491 A JP3298491 A JP 3298491A JP 3298491 A JP3298491 A JP 3298491A JP 2890863 B2 JP2890863 B2 JP 2890863B2
Authority
JP
Japan
Prior art keywords
polarization
degree
block
shaped piezoelectric
piezoelectric body
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP3298491A
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Japanese (ja)
Other versions
JPH04273186A (en
Inventor
幹雄 中島
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Murata Manufacturing Co Ltd
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Murata Manufacturing Co Ltd
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Priority to JP3298491A priority Critical patent/JP2890863B2/en
Publication of JPH04273186A publication Critical patent/JPH04273186A/en
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Publication of JP2890863B2 publication Critical patent/JP2890863B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Compositions Of Oxide Ceramics (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、ブロック状の圧電体を
分極する方法であって、特に、所望の分極度を簡単かつ
高精度に得ることができる分極方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method of polarizing a block-shaped piezoelectric material, and more particularly to a method of polarizing a desired degree of polarization with high accuracy.

【0002】[0002]

【従来の技術】図2は、厚みすべり振動モードを利用し
た従来より公知の圧電振動子を示す。圧電振動子1は、
矢印P方向に分極処理された圧電基板2の両主面に、圧
電基板2の中央部分で表裏対向するように電極3,4を
形成した構造を有する。この圧電振動子1は、図3に示
す工程に従って製造されている。
2. Description of the Related Art FIG. 2 shows a conventionally known piezoelectric vibrator utilizing a thickness shear vibration mode. The piezoelectric vibrator 1
It has a structure in which electrodes 3 and 4 are formed on both main surfaces of the piezoelectric substrate 2 polarized in the direction of the arrow P so as to face the front and back at the center of the piezoelectric substrate 2. This piezoelectric vibrator 1 is manufactured according to the process shown in FIG.

【0003】まず、ブロック状の圧電体5の両主面に分
極用電極6を形成する。次に、両主面に形成された分極
用電極6から高電圧を印加し、厚み方向に分極処理す
る。この分極は数万Vといったかなり高い電圧で行われ
る。従って、空気中で分極した場合には、放電等が生じ
危険であるため、通常、絶縁油中に圧電体5を浸漬した
状態で分極処理する。次に、図3に示すように、分極処
理された圧電体5をダイシング・ソーにより切断し、薄
板状の圧電母基板7を得る。さらに、得られた圧電母基
板7の両主面にマザーの電極3a,4aを形成した後、
図3の一点鎖線Aに沿って切断することにより図2の圧
電振動子1を得る。
[0003] First, polarization electrodes 6 are formed on both main surfaces of a block-shaped piezoelectric body 5. Next, a high voltage is applied from the polarization electrodes 6 formed on both main surfaces, and polarization is performed in the thickness direction. This polarization is performed at a considerably high voltage such as tens of thousands of volts. Therefore, when the polarization is performed in the air, a discharge or the like occurs, which is dangerous. Therefore, the polarization is usually performed in a state where the piezoelectric body 5 is immersed in the insulating oil. Next, as shown in FIG. 3, the polarized piezoelectric body 5 is cut by a dicing saw to obtain a thin plate-shaped piezoelectric mother substrate 7. Further, after forming mother electrodes 3a and 4a on both main surfaces of the obtained piezoelectric mother substrate 7,
The piezoelectric vibrator 1 of FIG. 2 is obtained by cutting along the dashed line A of FIG.

【0004】[0004]

【発明が解決しようとする課題】上記のように圧電振動
子1を量産するに当たっては、始めにブロック状の圧電
体5を厚み方向に分極処理していた。しかしながら、所
定の分極度を得るには、ブロック状という試料形状のた
めに数万Vといった高電圧を印加する必要があったた
め、絶縁油中に浸漬した状態で分極処理する必要があ
り、そのため分極処理後に絶縁油を除去するための煩雑
な洗浄作業が必要であった。
When the piezoelectric vibrator 1 is mass-produced as described above, the block-shaped piezoelectric body 5 is first polarized in the thickness direction. However, in order to obtain a predetermined degree of polarization, it was necessary to apply a high voltage of tens of thousands of volts due to the block shape of the sample, and thus it was necessary to perform a polarization treatment while immersing in insulating oil. A complicated cleaning operation for removing the insulating oil after the treatment was required.

【0005】また、上記のような製造工程を経て得られ
る圧電振動子1では、特性をそろえるには、ブロック状
圧電体5が一様にかつ高精度に分極処理されていること
が必要である。また、実際の量産に際しては、異なるブ
ロック状圧電体5を、等しい分極度を有するように、多
数のブロック状圧電体5を高精度にかつ安定に分極処理
する必要がある。
Further, in the piezoelectric vibrator 1 obtained through the above-described manufacturing process, it is necessary that the block-like piezoelectric body 5 is uniformly and highly accurately polarized in order to make the characteristics uniform. . Also, in actual mass production, it is necessary to stably polarize a large number of block-shaped piezoelectric members 5 with high accuracy so that different block-shaped piezoelectric members 5 have the same degree of polarization.

【0006】しかしながら、従来の分極方法では、圧電
材料のばらつき、焼成ロットの変動等により、圧電体5
の分極度にばらつきが生じざるを得なかった。その結
果、得られた圧電振動子1において、圧電基板2の分極
度がばらつくため、特性のばらつきの大きな原因となっ
ていた。のみならず、ブロック状圧電体5はかなりの厚
み及び寸法を有するため、上記のように数万Vと非常に
高い電圧を印加することにより分極していたが、このよ
うな高電圧を印加することによる分極では、分極度の制
御自体が非常に難しく、従ってブロック状圧電体5を一
様にかつ高精度に分極することは非常に困難であった。
[0006] However, in the conventional polarization method, the piezoelectric material 5 due to the variation of the piezoelectric material, the variation of the firing lot, and the like.
Inevitably had to vary in the degree of polarization. As a result, in the obtained piezoelectric vibrator 1, the degree of polarization of the piezoelectric substrate 2 varies, which is a major cause of the characteristic variation. Not only that, since the block-shaped piezoelectric body 5 has a considerable thickness and dimensions, it was polarized by applying a very high voltage of tens of thousands V as described above. In such a polarization, it is very difficult to control the degree of polarization itself, and thus it is very difficult to uniformly and accurately polarize the block-shaped piezoelectric body 5.

【0007】よって、本発明の目的は、比較的簡単な方
法でブロック状圧電体を均一にかつ高精度に分極し得る
方法を提供することにある。
Accordingly, an object of the present invention is to provide a method capable of uniformly and highly accurately polarizing a block-shaped piezoelectric body by a relatively simple method.

【0008】[0008]

【課題を解決するための手段】本発明は、ブロック状圧
電体の分極方法であり、ブロック状圧電体を任意の方向
に所望の分極度より強く分極する第1の分極工程と、前
記第1の分極工程とは逆方向に電圧を印加して分極反転
に至らないように、所望の分極度より弱く分極する第2
の分極工程と、第1の分極工程と同方向に電圧を印加し
分極度を高めることにより、所望の分極度を得る第3
の分極工程とを備えることを特徴とする。
SUMMARY OF THE INVENTION The present invention relates to a method for polarizing a block-shaped piezoelectric body, comprising: a first polarization step of polarizing the block-shaped piezoelectric body in a desired direction to a degree higher than a desired degree of polarization; Polarization inversion by applying a voltage in the opposite direction to the polarization process of
The second polarization, which is weaker than the desired degree of polarization so as not to reach
And a voltage in the same direction as the first polarization step.
By increasing the degree of polarization Te, third to obtain the desired degree of polarization
And a polarization step.

【0009】[0009]

【作用】本発明において、ブロック状圧電体を所望の分
極度に高精度に分極し得る理由は以下の通りである。一
般に、圧電体を分極する場合、または分極反転する場
合、抗電界以上の電圧を印加する必要がある。しかしな
がら、一度分極処理し、しかる後分極度を低下させ、さ
らに最初の分極方向に再度電圧を印加して分極度を高め
る場合には、非常に低い電圧で分極度を変化させること
ができることが本発明者により見出された。これは、最
初の分極処理の影響が残っていることによると考えら
れ、従って、低い電圧で分極度を高め得るので所望の分
極度を高精度に得ることができる。
In the present invention, the reason why the block-shaped piezoelectric body can be highly accurately polarized to a desired degree of polarization is as follows. Generally, when polarizing or reversing the polarization of a piezoelectric body, it is necessary to apply a voltage higher than the coercive electric field. However, in the case where the polarization is performed once, the degree of polarization is reduced, and then the voltage is applied again in the first polarization direction to increase the degree of polarization, it is important that the degree of polarization can be changed with a very low voltage. Found by the inventor. This is considered to be due to the effect of the initial polarization treatment remaining. Therefore, the degree of polarization can be increased at a low voltage, and a desired degree of polarization can be obtained with high accuracy.

【0010】なお、第1の分極工程における分極は、所
望の分極度より強く分極すればよく、例えば飽和分極状
態に分極してもよい。
The polarization in the first polarization step may be polarization stronger than a desired degree of polarization. For example, the polarization may be in a saturated polarization state.

【0011】[0011]

【実施例の説明】以下、本発明の具体的な実施例を説明
することにより本発明を明らかにする。ブロック状圧電
体として、Pb(TiZr)O3 系セラミックスよりな
り、プレス成形することにより20mm×30mm×厚
み7mmの寸法のものを用意した。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention will be clarified by describing specific embodiments of the present invention. As the block-shaped piezoelectric body, a piezoelectric body made of Pb (TiZr) O 3 -based ceramic and having a size of 20 mm × 30 mm × 7 mm in thickness was prepared by press molding.

【0012】上記ブロック状圧電体の両主面に、図3に
示したように分極用電極6を形成し、20kVの電圧を
80℃で1時間印加して分極処理し、飽和分極状態と
し、150℃の温度で1時間エージングした。この飽和
分極状態では、拡がり振動モード(短辺振動)について
の分極度ΔF=約9kHzであった(図1参照)。次
に、飽和分極状態とされたブロック状圧電体に、図1に
示すように上記第1の分極工程とは逆方向に電圧を印加
し、低分極状態とした。この場合、4種類のブロック状
圧電体を用意し、分極度が、それぞれ、ΔF=7.0
kHz、ΔF=5.0kHz、ΔF=3.0kHz
及びΔF=0.1kHzとなるように、それぞれ分極
処理した。
As shown in FIG. 3, a polarizing electrode 6 is formed on both main surfaces of the block-shaped piezoelectric body, and a voltage of 20 kV is applied at 80 ° C. for 1 hour to perform a polarization process to obtain a saturated polarization state. Aged at a temperature of 150 ° C. for 1 hour. In this saturated polarization state, the degree of polarization ΔF for the spreading vibration mode (short-side vibration) was about 9 kHz (see FIG. 1). Next, as shown in FIG. 1, a voltage was applied to the block-shaped piezoelectric body in the saturated polarization state in a direction opposite to that of the first polarization step, so that a low polarization state was obtained. In this case, four types of block-shaped piezoelectric bodies are prepared, and the degree of polarization is ΔF = 7.0, respectively.
kHz, ΔF = 5.0 kHz, ΔF = 3.0 kHz
And ΔF = 0.1 kHz.

【0013】なお、上記〜の分極度ΔFを実現する
には、上記の方法に変えて下記の方法を実施してもよ
い。(別法)20kVの電圧を80℃で1時間印加し、
次に逆電圧を印加して分極度を低下させた後、150℃
で1時間エージングする。この方法によれば、上記の方
法における第1回目及び第2回目の分極処理を一連の工
程で行い得る。
In order to realize the above-mentioned degree of polarization ΔF, the following method may be carried out instead of the above method. (Alternative method) A voltage of 20 kV is applied at 80 ° C. for 1 hour,
Next, after applying a reverse voltage to lower the degree of polarization,
Aging for 1 hour. According to this method, the first and second polarization treatments in the above method can be performed in a series of steps.

【0014】次に、低分極状態とされた4種類のブロッ
ク状圧電体に、それぞれ、再度順方向に電圧を印加し、
分極度を高めた。この場合、電圧の印加は図1の横軸の
印加電圧をxとした場合、xkV/7mm×80℃×1
0分の条件で行った。4種類のブロック状圧電体〜
のいずれにおいても、分極度が高められ、最終的には飽
和分極状態となった(図1参照)。
Next, a voltage is again applied in the forward direction to each of the four types of block-shaped piezoelectric materials in the low polarization state,
The degree of polarization was increased. In this case, when the applied voltage on the horizontal axis in FIG. 1 is x, xkV / 7 mm × 80 ° C. × 1
The test was performed under the condition of 0 minutes. Four types of block-shaped piezoelectric materials ~
In each case, the degree of polarization was increased, and eventually the state was saturated (see FIG. 1).

【0015】ところで、図1の分極度ΔF(kHz)と
印加電圧との関係から明らかなように、第3の分極工
程、すなわち最後に分極度を高めるように分極処理する
場合、その分極度−印加電圧曲線は第2の分極工程にお
いて分極度を低下させる場合に比べてかなりゆるやかな
ことが分かる。従って、例えばの例では、分極度5.
0kHzよりも高い分極度、例えば5.2〜5.6kH
Z付近の分極度を得ようとした場合、このような分極度
を高精度に実現し得ることが分かる。しかも、例えば
の例では、第3の分極工程を開始する場合において、ブ
ロック状圧電体は5.0kHzの分極度を有するため、
比較的低い電圧(5.2kHzの分極度を得ようとした
場合には800V、5.4kHzの分極度を得ようとし
た場合には1400V、5.6kHzの分極度を得よう
とした場合には2000V)を印加するだけで所望の分
極度に高め得ることが分かる。
By the way, as is clear from the relationship between the polarization degree ΔF (kHz) and the applied voltage in FIG. 1, in the third polarization step, that is, when the polarization processing is performed so as to finally increase the polarization degree, the polarization degree − It can be seen that the applied voltage curve is considerably gentler than when the degree of polarization is reduced in the second polarization step. Therefore, in the example, for example, the degree of polarization is 5.
Polarization degree higher than 0 kHz, for example, 5.2 to 5.6 kHz
It can be seen that when trying to obtain a degree of polarization near Z, such a degree of polarization can be realized with high accuracy. In addition, for example, in the case of starting the third polarization step, the block-shaped piezoelectric body has a polarization degree of 5.0 kHz,
A relatively low voltage (800 V when trying to obtain a polarization of 5.2 kHz, 1400 V when trying to obtain a polarization of 5.4 kHz, It can be seen that the desired degree of polarization can be increased only by applying 2000 V).

【0016】なお、第3の分極工程において分極度を高
める場合、上記のように印加電圧を高めて分極度を高め
るだけでなく、より低い印加電圧を印加し、かつ分極時
間を長くすることによって分極度を高めることも可能で
ある。すなわち、上記した実験例の場合、図4に示す
ように、1000V×80℃の条件で分極時間を延長す
れば、よりゆるやかに分極度を高め得ることが分かる。
従って、第3の分極工程において、より低い電圧を印加
し分極時間を延長することにより、分極度をより高精度
に制御し得ることが分かる。
When the degree of polarization is increased in the third polarization step, not only is the applied voltage increased as described above to increase the degree of polarization, but also by applying a lower applied voltage and lengthening the polarization time. It is also possible to increase the degree of polarization. That is, in the case of the above-described experimental example, as shown in FIG. 4, it is understood that the polarization degree can be more slowly increased by extending the polarization time under the condition of 1000 V × 80 ° C.
Therefore, it is understood that the degree of polarization can be controlled with higher precision by applying a lower voltage and extending the polarization time in the third polarization step.

【0017】上記のようにして分極処理されたブロック
状圧電体を用いて、図2に示した圧電振動子を多数作製
した。用いたブロック状圧電体の拡がり振動モードの分
極度ΔFと、作製された圧電振動子の圧電基板の厚みす
べり振動についての分極度Δfの関係を図5に示す。な
お、図5における実線B、破線C及び一点鎖線Dは、そ
れぞれ、異なる焼成ロットで得られたブロック状圧電体
から得られた複数の圧電振動子の特性の平均値を示す。
図5から明らかなように、いずれの焼成ロットのブロッ
ク状圧電体を用いても、ブロック状圧電体の分極度ΔF
と圧電振動子の圧電基板の分極度Δfとの間に同様の相
関があることが分かる。従って、本発明によれば、所望
の分極度を有する圧電部品を安定に供給し得ることが分
かる。
A large number of piezoelectric vibrators shown in FIG. 2 were manufactured using the block-shaped piezoelectric material subjected to the polarization treatment as described above. FIG. 5 shows the relationship between the polarization degree ΔF of the used block-shaped piezoelectric body in the spreading vibration mode and the polarization degree Δf of the manufactured piezoelectric vibrator with respect to the thickness shear vibration of the piezoelectric substrate. In addition, the solid line B, the broken line C, and the dashed-dotted line D in FIG. 5 indicate the average values of the characteristics of a plurality of piezoelectric vibrators obtained from the block-shaped piezoelectric bodies obtained in different firing lots.
As is clear from FIG. 5, the polarization degree ΔF of the block-shaped piezoelectric material was
It can be seen that there is a similar correlation between the degree of polarization Δf of the piezoelectric substrate of the piezoelectric vibrator. Therefore, according to the present invention, it can be seen that a piezoelectric component having a desired degree of polarization can be stably supplied.

【0018】[0018]

【発明の効果】以上のように、本発明のブロック状圧電
体の分極方法によれば、比較的低い電圧を印加すること
によりブロック状圧電体を均一にかつ高精度に分極する
ことが可能となる。しかも、第3の分極工程では低い電
圧を印加して分極し得るため、第3の分極工程を空気中
で行うことができ、従って分極作業も容易に行え得る。
よって、分極度の制御工程、すなわち第3の分極工程を
自動化することができ、圧電部品の量産性を飛躍的に高
めることが可能となる。
As described above, according to the method for polarizing a block-shaped piezoelectric body of the present invention, it is possible to uniformly and accurately polarize the block-shaped piezoelectric body by applying a relatively low voltage. Become. In addition, since a low voltage can be applied in the third polarization step to perform polarization, the third polarization step can be performed in air, and thus the polarization operation can be easily performed.
Therefore, the control step of the degree of polarization, that is, the third polarization step can be automated, and the mass productivity of piezoelectric components can be drastically improved.

【0019】また、ブロック状圧電体を高精度に分極し
得るため、該ブロック状圧電体から作製される圧電部品
の良品率を高めることも可能となる。
Further, since the block-shaped piezoelectric body can be polarized with high precision, it is possible to increase the yield rate of the piezoelectric components manufactured from the block-shaped piezoelectric body.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の実施例におけるブロック状圧電体の分
極度ΔFと印加電圧の関係を示す図である。
FIG. 1 is a diagram showing a relationship between a polarization degree ΔF of a block-shaped piezoelectric body and an applied voltage in an example of the present invention.

【図2】ブロック状圧電体から得られる圧電部品の一例
としての圧電振動子を示す斜視図である。
FIG. 2 is a perspective view showing a piezoelectric vibrator as an example of a piezoelectric component obtained from a block-shaped piezoelectric body.

【図3】ブロック状圧電体から図2の圧電振動子を得る
工程を説明するための各斜視図である。
3 is a perspective view for explaining a step of obtaining the piezoelectric vibrator of FIG. 2 from a block-shaped piezoelectric body.

【図4】第3の分極工程において、印加電圧を低めて分
極時間を延長した場合の分極度ΔFの変化を示す図であ
る。
FIG. 4 is a diagram showing a change in the degree of polarization ΔF when a polarization time is extended by reducing an applied voltage in a third polarization step.

【図5】ブロック状圧電体の分極度をΔFと該ブロック
状圧電体から得られた圧電振動子の圧電基板の分極度Δ
fとの関係を示す図である。
FIG. 5 shows the polarization degree of the block-shaped piezoelectric body ΔF and the polarization degree Δ of the piezoelectric substrate of the piezoelectric vibrator obtained from the block-shaped piezoelectric body.
It is a figure showing relation with f.

【符号の説明】[Explanation of symbols]

1 … 圧電振動子 2 … 圧電基板 3,4 … 電極 5 … ブロック状圧電体 6 … 分極用電極 7 … 圧電母基板 DESCRIPTION OF SYMBOLS 1 ... Piezoelectric vibrator 2 ... Piezoelectric substrate 3, 4 ... Electrode 5 ... Block-shaped piezoelectric body 6 ... Polarizing electrode 7 ... Piezoelectric mother board

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 ブロック状圧電体の分極方法であって、 前記ブロック状圧電体を任意の方向に所望の分極度より
強く分極する第1の分極工程と、 前記第1の分極工程とは逆方向に電圧を印加して分極反
転に至らないように、所望の分極度より弱く分極する第
2の分極工程と、 前記第1の分極工程と同方向に電圧を印加して分極度を
高めることにより、所望の分極度を得る第3の分極工程
とを備えることを特徴とするブロック状圧電体の分極方
法。
1. A method of polarizing a block-shaped piezoelectric body, comprising: a first polarization step of polarizing the block-shaped piezoelectric body in a desired direction to a degree larger than a desired degree of polarization; and a reverse of the first polarization step. Voltage in the direction
A second polarization step in which polarization is weaker than a desired degree of polarization so as not to cause inversion, and applying a voltage in the same direction as the first polarization step to reduce the degree of polarization .
And a third polarization step of obtaining a desired degree of polarization by increasing the polarization degree.
JP3298491A 1991-02-27 1991-02-27 Polarization method for block-shaped piezoelectric material Expired - Fee Related JP2890863B2 (en)

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JP3478227B2 (en) * 1999-08-03 2003-12-15 株式会社村田製作所 Polarization method of piezoelectric body
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